SYSTEMS AND ENGINEERING TECHNOLOGY INVESTIGATION OF AN INERTIAL CONFINEMENT FUSION-FISSION HYBRID REACTOR Kiranjit Mejer PTNR Research Project 2009 Frazer-Nash.

Slides:



Advertisements
Similar presentations
1 Controlled Fission 235 U + n X + Y + (~ 2.4) n Moderation of second generation neutrons Chain reaction. Water, D 2 O or graphite moderator. Ratio of.
Advertisements

Controlled Fission  235U + n  X + Y + (~2.4)n
Nuclear Technology Taming the nucleus?. Outline Controlled Fission Reactions. Fuel enrichment Neutron moderation Control rods Nuclear Plant Design and.
A2 Physics - L.O. Jones 2007 – Information gathered from Wikipedia Critical Mass.
SABR SUBCRITICAL ADVANCED BURNER REACTOR W. M. STACEY Georgia Tech FPA Symposium, Washington December, 2009.
Fuel Cycle Subcommittee: Overview and Status Fusion-Fission Hybrid Workshop Gaithersburg, MD September 30, 2009 Robert N. Hill Department Head – Nuclear.
Nuclear Power. Source: Uranium-235 Process: – An unstable uranium nucleus is bombarded with a neutron and splits into two smaller nuclei and some neutrons.
Nuclear Energy University Programs MS-RC1 - Reactor Concepts RD&D August 10, 2011 Christopher Grandy Argonne National Laboratory.
Transmutation (Objective 25
Characterization of the Engineering Test Reactor at the INL for Final Disposition TRTR 2007 J. R. Parry Irradiation Test Programs INL.
Views on Neutronics and Activation Issues Facing Liquid-Protected IFE Chambers L. El-Guebaly and the ARIES Team Fusion Technology Institute University.
Nuclear Energy E = mc 2 E: energy m: mass c: speed of light c = 3 x 10 8 m/s.
L. Tassan-Got – IPN Orsay Nuclear data and reactor physics Radiotoxicity and spent fuel.
Resent Breeding Blanket Experiments - CONTENTS - - Objectives - - Resent breeding design at JAERI - - Brief history of FNS blanket experiments - - Resent.
Safe and Abundant Energy from Accelerator-Driven Nuclear Fission by Alex Kiss.
Adam Smalley.  Describe how neutrons produced in a fission reaction may be used to initiate further fission reactions (chain reactions)  Distinguish.
Alternative Energy Sources
Development of the FW Mobile Tiles Concept Mohamed Sawan, Edward Marriott, Carol Aplin University of Wisconsin-Madison Lance Snead Oak Ridge National Laboratory.
UTILIZATION POSSIBILITIES OF THORIUM AS NUCLEAR FUEL Prof. Dr. Sümer ŞAHİN Atılım University Faculty of Engineering Department of Mechanical Engineering.
1 MCNP simulation of salt channel in LR-0 reactor 12th session of the AER Working Group F - "Spent Fuel Transmutations" and 3rd meeting of INPRO Project.
Nuclear Physics Year 13 Option 2006 Part 3 – Nuclear Fission.
Massimo Salvatores (CEA, Cadarache, France) WORKSHOP ON
Fundamentals of Neutronics : Reactivity Coefficients in Nuclear Reactors Paul Reuss Emeritus Professor at the Institut National des Sciences et Techniques.
Nuclear and Radiation Physics, BAU, 1 st Semester, (Saed Dababneh). 1 Nuclear Fission Q for 235 U + n  236 U is MeV. Table 13.1 in Krane:
Nuclear and Radiation Physics, BAU, First Semester, (Saed Dababneh). 1 Nuclear Fission 1/ v 235 U thermal cross sections  fission  584 b. 
Fusion-Fission Hybrid Systems
核工程计算物理实验室 Nuclear Engineering Computational Physics The Neutronics Studies of Fusion Fission Hybrid Power Reactor Youqi Zheng Ph. D Nuclear.
Team 16: The Nuclear Family EN-FISSIONING A SUSTAINABLE FUTURE.
Transmutations of Actinides in Fusion-Fission Hybrids – a Model Nuclear Synergy ? Stefan Taczanowski Faculty of Energy and Fuels AGH University of Science.
Section 24-3 Nuclear Fission Stability of elements is best around a mass number of 60. Atoms with a mass number greater than 60 tend to gain stability.
Fission and Fusion 3224 Nuclear and Particle Physics Ruben Saakyan UCL.
Fusion Blanket Technology
Neutronics Parameters for Preferred Chamber Configuration with Magnetic Intervention Mohamed Sawan Ed Marriott, Carol Aplin UW Fusion Technology Inst.
Future of Antiproton Triggered Fusion Propulsion Brice Cassenti & Terry Kammash University of Connecticut & University of Michigan.
Fission Physics 12 Adv. Comprehension Check 1. Two deuterium nuclei fuse to form a tritium nuclei and a proton. How much energy is liberated? 2. A deuterium.
The amount of carbon dioxide released (Kg CO 2 /kWh) annually in the UK. Do we need Nuclear Reactors?
Design Optimization of Toroidal Fusion Shield  Fusion Theory [BLAHBLAHBLAH] Fusion energy production is based on the collision nuclei in a deuterium and.
D J Coates, G T Parks Department of Engineering, University of Cambridge, UK Actinide Evolution and Equilibrium in Fast Thorium Reactors UNTF 2010 University.
A Fission-Fusion Hybrid Reactor in Steady-State L-Mode Tokamak Configuration with Natural Uranium Mark Reed FUNFI Varenna, Italy September 13 th, 2011.
1 Neutronics Assessment of Self-Cooled Li Blanket Concept Mohamed Sawan Fusion Technology Institute University of Wisconsin, Madison, WI With contributions.
Physics 12 Mr. Jean January 18 th, The plan: Video clip of the day Chapter 18 & 19 – MC.
Kayla J. Sax MPhil Candidate in Engineering Department of Engineering, University of Cambridge Supervised by Dr. Geoff T. Parks Investigating the Scope.
ThEC13, Geneva, 28th-31st Oct., 2013 C. H. Pyeon, Kyoto Univ. 1 Cheolho Pyeon Research Reactor Institute, Kyoto University, Japan
Characteristics of Transmutation Reactor Based on LAR Tokamak Neutron Source B.G. Hong Chonbuk National University.
Nuclear Reactors, BAU, 1st Semester, (Saed Dababneh).
Design optimization of Toroidal Fusion blanket/shield Basic Fusion Theory The basis for fusion energy production is to collide a deuterium and a tritium.
Controlled Nuclear Fusion The JET Project
Potential role of FF hybrids Massimo Salvatores CEA-Cadarache- France Fusion-Fission Hybrids have a potential role (in principle and independently from.
Nuclear Reactors, BAU, 1st Semester, (Saed Dababneh).
Nuclear Fission elementary principles
Why Thorium? # Thorium can address issues that have remained unresolved with Uranium based nuclear energy. * Thorium leads to some natural advantages in.
D J Coates, G T Parks Department of Engineering, University of Cambridge, UK 3 rd Year PhD student Actinide Breeding and Reactivity Variation in a Thermal.
The design of a hybrid FNS "fusion-fission" system for manufacture of artificial nuclear fuel and nuclide transmutation is actual [1-4]. At a stage of.
Neutron Chain Reaction Systems William D’haeseleer.
Controlling Nuclear Fission. Thermal neutrons Uranium 235 is the main fissile material which we are concerned with. Uranium-233 and plutonium-239 can.
Nuclear Power. Nuclear Fuel  Primarily involve nuclear fission  Fuel: typically is uranium-235 Must be enriched, as the most abundant isotope of uranium.
D J Coates, G T Parks Department of Engineering, University of Cambridge, UK Actinide Evolution and Equilibrium in Thorium Reactors ThorEA Workshop Trinity.
ADSR Workshop, May ‘08 ADSR Systems for Power Generation: some practical considerations Bob Cywinski 7 May 2008, Daresbury.
The tritium breeding blanket in Tokamak fusion reactors T. Onjun1), S. Sangaroon2), J. Prasongkit3), A. Wisitsorasak4), R. Picha5), J. Promping5) 1) Thammasat.
Summary of the Neutronics Analysis of Blankets for the Hybrid Fusion Neutron Source A.V.Zhirkin, B.V.Kuteev, M.I.Gurevich, B.K.Chukbar, NRC “Kurchatov.
What are fission and fusion? What fuels a nuclear reaction?
D J Coates, G T Parks Department of Engineering, University of Cambridge, UK Safety Considerations for the Design of Thorium Fueled ADS Reactors ThorEA.
Can We achieve the TBR Needed in FNF?
Toroidal Fusion Shielding Design Project
JOINT INSTITUTE FOR NUCLEAR RESEARCH
Pebble Bed Reactors for Once Trough Nuclear Transmutation
PARAMETRIC SURVEY OF COATED FUEL PARTICLE
Toroidal Fusion Shielding Design Project
Nuclear Reactors, BAU, 1st Semester, (Saed Dababneh).
Toroidal Fusion Shielding Design Project
Presentation transcript:

SYSTEMS AND ENGINEERING TECHNOLOGY INVESTIGATION OF AN INERTIAL CONFINEMENT FUSION-FISSION HYBRID REACTOR Kiranjit Mejer PTNR Research Project 2009 Frazer-Nash Consultancy University of Birmingham

© Frazer-Nash Consultancy Ltd All rights reserved. Confidential and proprietary document. SYSTEMS AND ENGINEERING TECHNOLOGY The Basic Concept  Fusion neutron source D + T → α + n MeV (n energy 14.1 MeV)  Sub critical fission blanket  Neutron multiplier blanket  Reflector Benefits of a Hybrid  Waste transmutation – reducing inventory of HLW  Production of energy  Development of fusion technology  Inherent safety The Fusion-Fission Hybrid Reactor

© Frazer-Nash Consultancy Ltd All rights reserved. Confidential and proprietary document. SYSTEMS AND ENGINEERING TECHNOLOGY Laser Inertial confinement Fusion-Fission Energy Engine  Inertial confinement fusion source  Surrounded by Beryllium blanket  Spherical blanket of sub-critical fission fuel  Graphite blanket  Pb-Li first wall coolant  FLiBe (2LiF+BeF 2 ) coolant  Power conversion system Image from ”Thermal and Mechanical Design Aspects of the LIFE Engine” R P Abbot et al, 2009

© Frazer-Nash Consultancy Ltd All rights reserved. Confidential and proprietary document. SYSTEMS AND ENGINEERING TECHNOLOGY Multiplication Factor of Be Blanket  Pure 9 Be – 1.85 gcm -3  Peak at 17 cm blanket thickness  Factor ~ 2.06  Pebble packing fraction 60 % gcm -3  Factor ~ 1.81 at 16 cm  Supported by “A Sustainable Nuclear Fuel Cycle Based on Laser Inertial Fusion Energy” Moses et al, 2009

© Frazer-Nash Consultancy Ltd All rights reserved. Confidential and proprietary document. SYSTEMS AND ENGINEERING TECHNOLOGY Fuel Blanket Investigation  Below - Energy gain from fission blanket of natural Uranium 19.1 gcm -3 surrounding a Beryllium blanket  Above - Energy gain from fission blanket of pure 238U

© Frazer-Nash Consultancy Ltd All rights reserved. Confidential and proprietary document. SYSTEMS AND ENGINEERING TECHNOLOGY Energy Spectrum of Neutrons  Neutron energy entering the fission blanket  ~ 0.05 at 14 MeV  Large proportion at thermal energies  Maxwell-Boltzmann distribution peaks at eV  Spectrum of neutrons returning from reflector shows same form

© Frazer-Nash Consultancy Ltd All rights reserved. Confidential and proprietary document. SYSTEMS AND ENGINEERING TECHNOLOGY Other Fuel Options radius 1 cm Outer radius 0.5 mmKernel radius 0.3 mm Buffer layer (C) High-densityPyc SiC coated particles embedded in graphite matrix 30% TRISO 70% Carbon  Fuel composition based on graphite pebbles containing TRISO particles Image adapted from

© Frazer-Nash Consultancy Ltd All rights reserved. Confidential and proprietary document. SYSTEMS AND ENGINEERING TECHNOLOGY Fission blanket energy gain and criticality Fuel optionFission Energy Gaink eff Th DU (0.26% 235 U) Natural U LWR Spent Nuclear Fuel Separated Transuranic Elements Weapons grade plutonium 2.342

© Frazer-Nash Consultancy Ltd All rights reserved. Confidential and proprietary document. SYSTEMS AND ENGINEERING TECHNOLOGY Coolant Effects  First wall coolant Pb 83 Li 17  Primary coolant FLiBe (2LiF + BeF 2 ) 6 Li + n → 4 He + T + Q 7 Li + n → 4 He + T + n’ – Q  Tritium Breeding Ratio (TBR) – ratio of T produced to consumed  For self sufficiency TBR > 1.05  Requires 6 Li enrichment of 50% or more

© Frazer-Nash Consultancy Ltd All rights reserved. Confidential and proprietary document. SYSTEMS AND ENGINEERING TECHNOLOGY Project Extensions Improvements to the Model  Geometry – structural materials etc  Fuel blanket compositions  Temperatures  Number of neutron histories  Other fuel fabrication options  Time dependent nature of the reactor - evolution of fuel with breeding from fertile isotopes - flattening power output with 6 Li content

© Frazer-Nash Consultancy Ltd All rights reserved. Confidential and proprietary document. SYSTEMS AND ENGINEERING TECHNOLOGY Summary  Demand for clean, abundant energy and concerns over HLW management have led to renewed interest in the hybrid concept  MCNP modelling has demonstrated the viability of a number of fuel options particularly SNF  Enrichment of 6 Li content in coolants can provide tritium self sufficiency for the reactor  Timescale for LIFE machine large

SYSTEMS AND ENGINEERING TECHNOLOGY

© Frazer-Nash Consultancy Ltd All rights reserved. Confidential and proprietary document. SYSTEMS AND ENGINEERING TECHNOLOGY MCNP Model  Isotropic, monoenergetic neutron point source  Pb-Li first wall coolant  Beryllium multiplier blanket  Fission Blanket  Graphite reflector  Stochastic approach - uses random number generation and reaction cross section data to determine the ‘history’ of a particle  Many histories followed to give a representation of a real world situation

© Frazer-Nash Consultancy Ltd All rights reserved. Confidential and proprietary document. SYSTEMS AND ENGINEERING TECHNOLOGY